Hochschild cohomology
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\documentclass{article} \usepackage{amsmath,amsfonts,amssymb,epsfig,color} \newcommand{\C}{\mathbb{C}} \newcommand{\Z}{\mathbb{Z}} \newcommand{\R}{\mathbb{R}} \newcommand{\iso}{\cong} \parskip1em \parindent0em \begin{document} \underline{Hochschild cohomology} Hochschild cohomology is tied up with the very basics of $A_\infty$-structures, but it also plays a more direct role in Fukaya categories through ``bulk deformations''. This talk has two kinds of prerequisites: one is the knowledge of Hochschild cohomology at least as it appears in the deformation theory of algebras, and the other one is some knowledge of Fukaya categories. There are few references apart from the inevitable [Fukaya-Oh-Ohta-Ono, book] and the papers by the same authors on toric varieties. \underline{Plan} {\it Definition.} We start with the Hochschild complex of an ordinary graded algebra, and the Lie bracket on that complex. There are many references, such as the book [Hazewinkel et al, eds., Deformation of algebras and structures and applications]. The $A_\infty$-structure equation appears as Maurer-Cartan equation in the resulting dg Lie algebra, which is relevant for deformation theory. In particular, it explains a phenomenon called intrinsic formality: under suitable vanishing conditions on the Hochschild cohomology of an algebra, every $A_\infty$-deformation of that algebra is isomorphic to the trivial one. You'll find a discussion in [Seidel-Thomas, braid group actions on derived categories of coherent sheaves]. As an example, the Hochschild-Kostant-Rosenberg theorem on the Hochschild cohomology of polynomial algebras can serve. It also illustrates the two structures present on Hochschild cohomology (Lie bracket and product). {\it Generalization.} More generally, one can consider the Hochschild cohomology of an $A_\infty$-algebra. This is actually obvious from the Maurer-Cartan framework above. Less obvious is the fact that we still have the commutative product (that becomes straightforward if one thinks in terms of bimodules, but we'd problably best avoid that). Hochschild cohomology still governs formal deformations of the $A_\infty$-structure. {\it Application.} For any symplectic manifold $M$, there is a ring homomorphism \[ QH^*(M) \longrightarrow HH^*(\mathcal F,\mathcal F) \] from the quantum cohomology ring to the Hochschild cohomology of the Fukaya category. This is defined by considering discs with an interior marked point, and one can interpret it in deformation theory terms: (generalized) infinitesimal deformations of the symplectic form induce deformations of the Fukaya category. It is instructive to see an informal (picture) proof of the fact that the map above is compatible with the ring structure. \underline{Notes} For attempts to generalize the above homomorphism to other contexts, see [Seidel, Fukaya categories and deformations] (non-compact manifolds; somewhat unsuccessful), and [Seidel, More about vanishing cycles and mutations]. \underline{Dependencies} Depends on having defined the Fukaya category, and also I think on the talk about quantum cohomology. \end{document}
